Esempio n. 1
0
func ExampleTimes() {
	// Example 15.a, p. 103.
	// Venus on 1988 March 20
	p := globe.Coord{
		Lon: unit.NewAngle(' ', 71, 5, 0),
		Lat: unit.NewAngle(' ', 42, 20, 0),
	}
	Th0 := unit.NewTime(' ', 11, 50, 58.1)
	α3 := []unit.RA{
		unit.NewRA(2, 42, 43.25),
		unit.NewRA(2, 46, 55.51),
		unit.NewRA(2, 51, 07.69),
	}
	δ3 := []unit.Angle{
		unit.NewAngle(' ', 18, 02, 51.4),
		unit.NewAngle(' ', 18, 26, 27.3),
		unit.NewAngle(' ', 18, 49, 38.7),
	}
	h0 := unit.AngleFromDeg(-.5667)
	ΔT := unit.Time(56)
	tRise, tTransit, tSet, err := rise.Times(p, ΔT, h0, Th0, α3, δ3)
	if err != nil {
		fmt.Println(err)
		return
	}
	fmt.Printf("rising:  %+.5f %02s\n", tRise/86400, sexa.FmtTime(tRise))
	fmt.Printf("transit: %+.5f %02s\n", tTransit/86400, sexa.FmtTime(tTransit))
	fmt.Printf("seting:  %+.5f %02s\n", tSet/86400, sexa.FmtTime(tSet))
	// Output:
	// rising:  +0.51766  12ʰ25ᵐ26ˢ
	// transit: +0.81980  19ʰ40ᵐ30ˢ
	// seting:  +0.12130  02ʰ54ᵐ40ˢ
}
Esempio n. 2
0
func ExampleTimes_computed() {
	// Example 15.a, p. 103, but using meeus packages to compute values
	// given in the text.
	jd := julian.CalendarGregorianToJD(1988, 3, 20)
	p := globe.Coord{
		Lon: unit.NewAngle(' ', 71, 5, 0),
		Lat: unit.NewAngle(' ', 42, 20, 0),
	}
	// Th0 computed rather than taken from the text.
	Th0 := sidereal.Apparent0UT(jd)

	// Venus α, δ computed rather than taken from the text.
	e, err := pp.LoadPlanet(pp.Earth)
	if err != nil {
		fmt.Println(err)
		return
	}
	v, err := pp.LoadPlanet(pp.Venus)
	if err != nil {
		fmt.Println(err)
		return
	}
	α := make([]unit.RA, 3)
	δ := make([]unit.Angle, 3)
	α[0], δ[0] = elliptic.Position(v, e, jd-1)
	α[1], δ[1] = elliptic.Position(v, e, jd)
	α[2], δ[2] = elliptic.Position(v, e, jd+1)
	for i, j := range []float64{jd - 1, jd, jd + 1} {
		_, m, d := julian.JDToCalendar(j)
		fmt.Printf("%s %.0f  α: %0.2s  δ: %0.1s\n",
			time.Month(m), d, sexa.FmtRA(α[i]), sexa.FmtAngle(δ[i]))
	}

	// ΔT computed rather than taken from the text.
	ΔT := deltat.Interp10A(jd)
	fmt.Printf("ΔT: %.1f\n", ΔT)

	h0 := rise.Stdh0Stellar
	tRise, tTransit, tSet, err := rise.Times(p, ΔT, h0, Th0, α, δ)
	if err != nil {
		fmt.Println(err)
		return
	}
	fmt.Printf("rising:   %+.5f %02s\n", tRise/86400, sexa.FmtTime(tRise))
	fmt.Printf("transit:  %+.5f %02s\n", tTransit/86400, sexa.FmtTime(tTransit))
	fmt.Printf("seting:   %+.5f %02s\n", tSet/86400, sexa.FmtTime(tSet))
	// Output:
	// March 19  α: 2ʰ42ᵐ43.25ˢ  δ: 18°02′51.4″
	// March 20  α: 2ʰ46ᵐ55.51ˢ  δ: 18°26′27.3″
	// March 21  α: 2ʰ51ᵐ07.69ˢ  δ: 18°49′38.7″
	// ΔT: 55.9
	// rising:   +0.51766  12ʰ25ᵐ26ˢ
	// transit:  +0.81980  19ʰ40ᵐ30ˢ
	// seting:   +0.12130  02ʰ54ᵐ40ˢ
}
Esempio n. 3
0
func ExampleTimes() {
	// Example 15.a, p. 103.
	jd := julian.CalendarGregorianToJD(1988, 3, 20)
	p := globe.Coord{
		Lon: base.NewAngle(false, 71, 5, 0).Rad(),
		Lat: base.NewAngle(false, 42, 20, 0).Rad(),
	}
	// Meeus gives us the value of 11h 50m 58.1s but we have a package
	// function for this:
	Th0 := sidereal.Apparent0UT(jd)
	α3 := []float64{
		base.NewRA(2, 42, 43.25).Rad(),
		base.NewRA(2, 46, 55.51).Rad(),
		base.NewRA(2, 51, 07.69).Rad(),
	}
	δ3 := []float64{
		base.NewAngle(false, 18, 02, 51.4).Rad(),
		base.NewAngle(false, 18, 26, 27.3).Rad(),
		base.NewAngle(false, 18, 49, 38.7).Rad(),
	}
	h0 := rise.Stdh0Stellar
	// Similarly as with Th0, Meeus gives us the value of 56 for ΔT but
	// let's use our package function.
	ΔT := deltat.Interp10A(jd)
	rise, transit, set, err := rise.Times(p, ΔT, h0, Th0, α3, δ3)
	if err != nil {
		fmt.Println(err)
		return
	}
	fmt.Println("rising: ", base.NewFmtTime(rise))
	fmt.Println("transit:", base.NewFmtTime(transit))
	fmt.Println("seting: ", base.NewFmtTime(set))
	// Output:
	// rising:  12ʰ26ᵐ9ˢ
	// transit: 19ʰ40ᵐ30ˢ
	// seting:  2ʰ54ᵐ26ˢ
}